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and Cosmology

Extragalactic Astronomy and Cosmology: An Introduction

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7.5 Non-Linear Structure Evolution<br />

Combining (7.37) <strong>and</strong> (7.38), we can express the halo<br />

mass <strong>and</strong> virial radius as a function of the virial velocity,<br />

M = V 3 200<br />

10GH(z) , r 200 = V 200<br />

10H(z) . (7.39)<br />

Since the Hubble function H(z) increases with redshift,<br />

the virial radius at fixed virial velocity decreases with<br />

redshift. From (7.37) we also see that r 200 decreases<br />

with redshift at fixed halo mass. Hence, halos at a given<br />

mass (or given virial velocity) are more compact at<br />

higher redshift than they are today.<br />

The NFW Profile. The density profile of halos averaged<br />

over spherical shells seems to have a universal functional<br />

form, which was first reported by Julio Navarro,<br />

Carlos Frenk & Simon White in a series of articles in<br />

the mid-1990s. This NFW-profile is described by<br />

ρ(r) =<br />

ρ s<br />

(r/r s )(1 +r/r s ) 2 , (7.40)<br />

where ρ s is the amplitude of the density profile, <strong>and</strong><br />

r s specifies a characteristic radius. For r ≪ r s we find<br />

ρ ∝ r −1 , whereas for r ≫ r s , the profile follows ρ ∝ r −3 .<br />

Therefore, r s is the radius at which the slope of the density<br />

profile changes (see Fig. 7.13). ρ s can be expressed<br />

in terms of r s , since, according to the definition of r 200 ,<br />

ρ = 200ρ cr (z) = 3<br />

4πr 3 200<br />

∫1<br />

= 3ρ s<br />

0<br />

∫<br />

r 200<br />

0<br />

4πr 2 dr ρ(r)<br />

dx x 2<br />

cx(1 + cx) 2 , (7.41)<br />

where in the last step the integration variable was<br />

changed to x = r/r 200 , <strong>and</strong> the concentration index<br />

c := r 200<br />

r s<br />

(7.42)<br />

was defined. The larger the value of c, the more strongly<br />

the mass is concentrated towards the inner regions.<br />

299<br />

Fig. 7.13. For eight different cosmological<br />

simulations, the density profile is shown for<br />

the most massive <strong>and</strong> the least massive halo,<br />

each as a function of the radius, together<br />

with the best fitting density profile (7.40).<br />

The cosmological models represent an EdS<br />

model (here denoted by SCDM), a ΛCDM<br />

model, <strong>and</strong> different models with power<br />

spectra that are assumed to be power laws<br />

locally, P(k) ∝ k n . The arrows indicate the<br />

softening length in the gravitational force<br />

for the respective halos; thus, the major part<br />

of the profiles is numerically well resolved

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